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arxiv: 2605.04586 · v1 · submitted 2026-05-06 · ✦ hep-th

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Bound states and deconfinement from Romans supergravity with magnetic flux

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Pith reviewed 2026-05-08 17:30 UTC · model grok-4.3

classification ✦ hep-th
keywords holographysupergravityconfinementdeconfinementphase transitionbound statesmagnetic fluxdilaton
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The pith

Romans supergravity solutions with magnetic flux exhibit a zero-temperature first-order deconfinement transition and two nearly degenerate light scalar bound states.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines the spectrum of bound states in a one-parameter family of strongly coupled confining four-dimensional field theories using their holographic duals. These duals are regular non-supersymmetric solutions of six-dimensional Romans supergravity that include a non-trivial Abelian magnetic flux. The solutions display a first-order phase transition at zero temperature from a confined to a deconfined phase when the flux strength reaches a critical upper limit that the geometry can support. Fluctuations around the backgrounds yield a spectrum in which two scalars are the lightest particles, with masses suppressed and almost degenerate for all parameter values; away from the transition the heavier scalar behaves as a dilaton while near the transition the scalars mix and their masses become parametrically smaller.

Core claim

The central claim is that the one-parameter family of background solutions ends in a zero-temperature deconfinement first-order phase transition triggered by the magnetic flux, which therefore sets an upper bound on the flux magnitude that can be supported. The spectrum of fluctuations of the background fields reveals two scalar particles as the lightest in the spectrum, their masses suppressed and almost degenerate across the whole parameter space. Away from the transition the heaviest of these two is identified as a dilaton, the pseudo-Nambu-Goldstone boson associated with scale invariance that couples to the trace of the stress-energy tensor of the dual field theory, while the lightest of

What carries the argument

The one-parameter family of regular non-supersymmetric background solutions of Romans half-maximal supergravity in six dimensions with non-trivial Abelian magnetic flux, which serve as holographic duals to the confining theories and allow extraction of the bound-state spectrum from linear fluctuations of the metric and fields.

If this is right

  • The magnetic flux strength sets an upper bound on the magnitude supportable by the geometry before the first-order deconfinement transition occurs.
  • Two scalar particles remain the lightest in the spectrum and stay almost degenerate for every value of the flux parameter.
  • Away from the transition the heavier light scalar is the dilaton that couples to the trace of the stress-energy tensor.
  • Near the critical flux a high-curvature region appears and the two scalars mix, making their masses parametrically smaller than those of other bound states.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • This construction gives an explicit example in which an external flux parameter directly controls the onset of deconfinement in a holographic model.
  • The parametric mass suppression near the transition suggests that additional light degrees of freedom may appear in the dual theory when the geometry develops large curvature.
  • The clean separation between the dilaton and the other light scalar away from the transition offers a controlled setting to study the trace anomaly in confining theories.
  • Stability of the backgrounds against higher-curvature corrections becomes especially important in the region close to the transition.

Load-bearing premise

The regular background solutions are valid and correctly identified as holographic duals to four-dimensional confining field theories, and the linear fluctuation analysis around them gives the bound-state spectrum without significant back-reaction or higher-derivative corrections.

What would settle it

A direct evaluation of the on-shell gravitational action that shows the free energy is continuous rather than discontinuous at the critical flux value, or a spectrum computation in which the two scalars are not the lightest states or lack the reported near-degeneracy.

Figures

Figures reproduced from arXiv: 2605.04586 by Ali Fatemiabhari, Maurizio Piai.

Figure 1
Figure 1. Figure 1: FIG. 1: The Ricci scalar, view at source ↗
Figure 2
Figure 2. Figure 2: displays our results for the dimensionless free energy density, Fˆ, computed for the solutions with non￾trivial flux, as a function of the dimensionless deforming parameter A (3),U 6 . In the case of the AdS6, domain-wall solutions with trivial (constant) flux, the prescription in Eq. (82) yields F = 0, and these solutions exist for any choice of A (3),U 6 . The figure demonstrates the existence of a first… view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: Ratio, view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Spectrum of masses, view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Spectrum of masses, view at source ↗
read the original abstract

We apply the dictionary of gauge-gravity dualities to study the spectrum of bound states in a special one-parameter family of strongly coupled, confining field theories in four dimensions. The top-down, holographic gravity dual description of this class of theories has been identified recently. It consists of non-supersymmetric regular background solutions of Romans half-maximal supergravity theory in six dimensions, in the presence of a non-trivial Abelian magnetic flux along a compactified direction of the geometry. A zero-temperature, deconfinement, first-order phase transition appears at one end of this branch of solutions. It is triggered by the strength of the flux, setting an upper bound on the magnitude of the magnetic flux that can be supported by the geometry. We compute the spectrum of fluctuations of the background fields in the gravity description, that correspond to field-theory bound states. Two scalar particles are the lightest in the spectrum, their masses being suppressed and almost degenerate across the whole parameter space. Away from the transition, the heaviest between these two particles is identified as a dilaton, the pseudo-Nambu-Goldstone boson associated with scale invariance. It couples to the trace of the stress-energy tensor of the dual field theory, while the lightest scalar does not. In the range of parameter space closest to the extremum of the one-parameter family, near the first-order phase transition, a region with large curvature appears at the end of space of the geometry of the solutions. In this range, the two scalars mix non-trivially, and their masses are parametrically suppressed, in respect to the other bound states.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript constructs a one-parameter family of non-supersymmetric regular backgrounds in six-dimensional Romans supergravity with non-trivial Abelian magnetic flux, proposed as holographic duals to a class of confining four-dimensional field theories. It identifies a zero-temperature first-order deconfinement phase transition at a critical flux strength that bounds the allowable flux. Linearized fluctuations around these backgrounds are solved to extract the bound-state spectrum, finding two lightest scalars that remain nearly degenerate and parametrically suppressed across the parameter space, with non-trivial mixing near the transition; away from the transition the heavier of the two is identified as a dilaton coupling to the trace of the stress-energy tensor.

Significance. If the classical supergravity approximation remains valid, the work supplies a concrete top-down holographic setup in which a tunable magnetic flux controls a deconfinement transition and generates parametrically light scalar bound states, including an explicit dilaton identification. The explicit construction of the backgrounds and the numerical extraction of the fluctuation spectrum constitute the main strengths.

major comments (2)
  1. [§4] §4 (background solutions near the extremum): the manuscript states that 'a region with large curvature appears at the end of space' in the range closest to the first-order transition, yet provides no quantitative estimate of the curvature radius in string units as a function of the flux parameter. This is load-bearing because the reported parametric suppression of the two scalar masses and their non-trivial mixing occur precisely in this high-curvature regime.
  2. [§5.1] §5.1 (fluctuation spectrum): the linearized equations for the scalar fluctuations assume the classical 6D supergravity background remains reliable; without a check that the string-frame curvature invariants stay ≪ 1/α' near the endpoint, the extracted mass eigenvalues and mixing angles cannot be trusted in the regime where the suppression is claimed.
minor comments (2)
  1. [Abstract and §3] The abstract and §3 could include a brief statement of the numerical method and convergence criteria used to generate the one-parameter family of solutions.
  2. [§2] Notation for the magnetic flux strength parameter is introduced without an explicit equation reference in the early sections; a single defining equation would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and the constructive comments. We address each major point below and indicate the revisions that will be incorporated to strengthen the presentation of the results.

read point-by-point responses
  1. Referee: [§4] §4 (background solutions near the extremum): the manuscript states that 'a region with large curvature appears at the end of space' in the range closest to the first-order transition, yet provides no quantitative estimate of the curvature radius in string units as a function of the flux parameter. This is load-bearing because the reported parametric suppression of the two scalar masses and their non-trivial mixing occur precisely in this high-curvature regime.

    Authors: We agree that a quantitative estimate of the curvature radius (in string units) as a function of the flux parameter is necessary to assess the regime of validity of the classical supergravity approximation. The manuscript notes the appearance of large curvature near the endpoint but does not provide the requested estimate. In the revised version we will compute and plot the relevant curvature invariants (including the string-frame Ricci scalar and higher invariants) evaluated at the endpoint, as functions of the flux parameter. This will allow us to identify the range of parameters where the curvature radius remains parametrically larger than the string length and where the reported parametric suppression of the scalar masses can be reliably interpreted within the supergravity framework. revision: yes

  2. Referee: [§5.1] §5.1 (fluctuation spectrum): the linearized equations for the scalar fluctuations assume the classical 6D supergravity background remains reliable; without a check that the string-frame curvature invariants stay ≪ 1/α' near the endpoint, the extracted mass eigenvalues and mixing angles cannot be trusted in the regime where the suppression is claimed.

    Authors: We acknowledge that the linearized fluctuation analysis is performed within the classical supergravity limit and that its reliability near the endpoint requires explicit verification that string-frame curvature invariants remain much smaller than 1/α'. The current manuscript does not contain such a check. In the revision we will add a dedicated subsection (or appendix) that evaluates the string-frame curvature invariants along the background solutions, particularly near the endpoint, and demonstrates that they satisfy the required bound in the parameter range where the two lightest scalars remain parametrically light and exhibit non-trivial mixing. This will directly support the trustworthiness of the reported mass eigenvalues and mixing angles. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation proceeds from direct solution of EOM and standard fluctuation analysis

full rationale

The paper constructs the one-parameter family of backgrounds by solving the equations of motion of six-dimensional Romans supergravity in the presence of magnetic flux, identifies the endpoint of the branch (and associated first-order transition) from the geometry of those solutions, and extracts the bound-state spectrum by linearizing fluctuations around the backgrounds. These steps are independent applications of the supergravity action and the gauge-gravity dictionary; they do not reduce by construction to fitted parameters renamed as predictions, nor do they rest on load-bearing self-citations whose content is unverified. The recent identification of the dual is used for context but is not invoked to force uniqueness or to substitute for the explicit computations performed here.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The analysis rests on the standard holographic dictionary, the validity of the supergravity approximation, and the assumption that the chosen magnetic-flux ansatz yields regular confining geometries; no new entities are postulated beyond the usual supergravity fields.

free parameters (1)
  • magnetic flux strength parameter
    The one-parameter family is controlled by the magnitude of the Abelian magnetic flux; its critical value that triggers the phase transition is determined numerically from the geometry.
axioms (2)
  • domain assumption Romans half-maximal supergravity in six dimensions admits regular non-supersymmetric solutions with magnetic flux along a compact direction that are dual to confining 4D field theories.
    Invoked throughout the abstract as the starting point for the holographic dictionary.
  • domain assumption Linearized fluctuations of the supergravity fields around the background correspond to the spectrum of bound states in the dual field theory.
    Standard assumption of the gauge-gravity duality used to extract masses.

pith-pipeline@v0.9.0 · 5585 in / 1708 out tokens · 31421 ms · 2026-05-08T17:30:28.289094+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

183 extracted references · 168 canonical work pages · 5 internal anchors

  1. [1]

    In performing the numerical calculations, we adopt the mid-point determinant, as in Ref. [77]. We scan numerically over the values ofM 2, in the presence of explicit cutoffsϱ 0 < ϱ 1 < ϱ < ϱ 2 <+∞, by imposing the boundary conditions in Eq. (99) at the two cutoffs, evolving the solutions of Eq. (98) to an intermediate value of the radial direction,ϱ ∗, co...

  2. [2]

    Third, two of the scalar towers become approximately degenerate

    Second, the mass of the lightest vector tend to vanish as well, in the same limit. Third, two of the scalar towers become approximately degenerate. This might be related to symmetry enhancement, but unfortunately the limiting caseϱ 0 = 3 4 is singular. Understanding the features of the spectrum in this region of parameter space may require going beyond th...

  3. [3]

    The only exception is the caseϱ 0 = 3 4, for which both (inequivalent) confining and conformal vacua have vanishing free energy

    We confirmed that these solutions correspond to confining field theories with vacuum free energy lower than the associated conformal field theories obtained with the same deformation parameters. The only exception is the caseϱ 0 = 3 4, for which both (inequivalent) confining and conformal vacua have vanishing free energy. The coexistence of phases is a st...

  4. [4]

    Gauge invariant formalism for the fluctuations The equations that govern the gauge-invariant treatment of the fluctuations are taken from Refs. [75–83]. We rewrite the general scalar, Φ a, by splitting it in background and (small) fluctuations, following Refs. [75–79], to read: Φa(xµ, r) = Φ a(r) +φ a(xµ, r),(A10) whereφ a(xµ, r) are small fluctuations ar...

  5. [5]

    For simplicity, we write the equation in the coordinater, although in the numerical study we performed we used the change of variable toϱ

    Equations of motion for fluctuations In this Appendix, we write explicitly the equations of motion for the fluctuations of the scalars, both in gauge- invariant form, and in the probe approximation. For simplicity, we write the equation in the coordinater, although in the numerical study we performed we used the change of variable toϱ. We also find it con...

  6. [6]

    IR expansions We find it convenient to write the expansions in the IR in the variableϱ. The leading terms of the IR expansion, in powers of the small quantityϱ−ϱ 0, of the scalar fluctuations are given by the following expressions: aϕ IR(ϱ) =aϕ IR,0 +a ϕ IR,L log(ϱ−ϱ 0)+ (ϱ−ϱ 0) 6ϱ5/2 0 (4ϱ0 −3) " aϕ IR,0 ϱ3/2 0 −2M2 + 88ϱ2 0 −174ϱ 0 + 81 + 2aϕ IR,L ϱ3/2 ...

  7. [7]

    We find it convenient to write the expansion at asymptotically large values ofϱas powers of a fifth way to parametrise the holographic direction, by definingz≡ 1 ϱ

    UV expansions We collect here the UV expansions, truncated to the first few terms, for all the spin-0 and spin-1 fluctuations of the soliton solutions with non-trivial flux. We find it convenient to write the expansion at asymptotically large values ofϱas powers of a fifth way to parametrise the holographic direction, by definingz≡ 1 ϱ. For the three gaug...

  8. [8]

    The Large N Limit of Superconformal Field Theories and Supergravity

    J.M. Maldacena,The Large N limit of superconformal field theories and supergravity,Adv. Theor. Math. Phys.2(1998) 231 [hep-th/9711200]

  9. [9]

    Gauge Theory Correlators from Non-Critical String Theory

    S.S. Gubser, I.R. Klebanov and A.M. Polyakov,Gauge theory correlators from noncritical string theory,Phys. Lett. B 428(1998) 105 [hep-th/9802109]

  10. [10]

    Anti De Sitter Space And Holography

    E. Witten,Anti-de Sitter space and holography,Adv. Theor. Math. Phys.2(1998) 253 [hep-th/9802150]

  11. [11]

    Large N Field Theories, String Theory and Gravity

    O. Aharony, S.S. Gubser, J.M. Maldacena, H. Ooguri and Y. Oz,Large N field theories, string theory and gravity,Phys. Rept.323(2000) 183 [hep-th/9905111]. 31

  12. [12]

    Anti-de Sitter Space, Thermal Phase Transition, And Confinement In Gauge Theories

    E. Witten,Anti-de Sitter space, thermal phase transition, and confinement in gauge theories,Adv. Theor. Math. Phys.2 (1998) 505 [hep-th/9803131]

  13. [13]

    Wen and H.-X

    C.-K. Wen and H.-X. Yang,QCD(4) glueball masses from AdS(6) black hole description,Mod. Phys. Lett. A20(2005) 997 [hep-th/0404152]

  14. [14]

    Kuperstein and J

    S. Kuperstein and J. Sonnenschein,Non-critical, near extremal AdS(6) background as a holographic laboratory of four dimensional YM theory,JHEP11(2004) 026 [hep-th/0411009]

  15. [15]

    Brower, S.D

    R.C. Brower, S.D. Mathur and C.-I. Tan,Glueball spectrum for QCD from AdS supergravity duality,Nucl. Phys. B587 (2000) 249 [hep-th/0003115]

  16. [16]

    Elander, A.F

    D. Elander, A.F. Faedo, C. Hoyos, D. Mateos and M. Piai,Multiscale confining dynamics from holographic RG flows, JHEP05(2014) 003 [1312.7160]

  17. [17]

    Chamseddine and M.S

    A.H. Chamseddine and M.S. Volkov,NonAbelian BPS monopoles in N=4 gauged supergravity,Phys. Rev. Lett.79 (1997) 3343 [hep-th/9707176]

  18. [18]

    Klebanov and M.J

    I.R. Klebanov and M.J. Strassler,Supergravity and a confining gauge theory: Duality cascades and chi SB resolution of naked singularities,JHEP08(2000) 052 [hep-th/0007191]

  19. [19]

    Maldacena and C

    J.M. Maldacena and C. Nunez,Towards the large N limit of pure N=1 superYang-Mills,Phys. Rev. Lett.86(2001) 588 [hep-th/0008001]

  20. [20]

    Butti, M

    A. Butti, M. Grana, R. Minasian, M. Petrini and A. Zaffaroni,The Baryonic branch of Klebanov-Strassler solution: A supersymmetric family of SU(3) structure backgrounds,JHEP03(2005) 069 [hep-th/0412187]

  21. [21]

    Dymarsky, I.R

    A. Dymarsky, I.R. Klebanov and N. Seiberg,On the moduli space of the cascading SU(M+p) x SU(p) gauge theory, JHEP01(2006) 155 [hep-th/0511254]

  22. [22]

    Andrews and N

    R.P. Andrews and N. Dorey,Deconstruction of the Maldacena-Nunez compactification,Nucl. Phys. B751(2006) 304 [hep-th/0601098]

  23. [23]

    Hoyos-Badajoz, C

    C. Hoyos-Badajoz, C. Nunez and I. Papadimitriou,Comments on the String dual to N=1 SQCD,Phys. Rev. D78 (2008) 086005 [0807.3039]

  24. [24]

    Nunez, I

    C. Nunez, I. Papadimitriou and M. Piai,Walking Dynamics from String Duals,Int. J. Mod. Phys. A25(2010) 2837 [0812.3655]

  25. [25]

    Elander, C

    D. Elander, C. Nunez and M. Piai,A Light scalar from walking solutions in gauge-string duality,Phys. Lett. B686 (2010) 64 [0908.2808]

  26. [26]

    Cassani and A.F

    D. Cassani and A.F. Faedo,A Supersymmetric consistent truncation for conifold solutions,Nucl. Phys. B843(2011) 455 [1008.0883]

  27. [27]

    I. Bena, G. Giecold, M. Grana, N. Halmagyi and F. Orsi,Supersymmetric Consistent Truncations of IIB onT 1,1,JHEP 04(2011) 021 [1008.0983]

  28. [28]

    Bennett, E

    S. Bennett, E. Caceres, C. Nunez, D. Schofield and S. Young,The Non-SUSY Baryonic Branch: Soft Supersymmetry Breaking of N=1 Gauge Theories,JHEP05(2012) 031 [1111.1727]

  29. [29]

    Dymarsky and S

    A. Dymarsky and S. Kuperstein,Non-supersymmetric Conifold,JHEP08(2012) 033 [1111.1731]

  30. [30]

    Maldacena and D

    J. Maldacena and D. Martelli,The Unwarped, resolved, deformed conifold: Fivebranes and the baryonic branch of the Klebanov-Strassler theory,JHEP01(2010) 104 [0906.0591]

  31. [31]

    Gaillard, D

    J. Gaillard, D. Martelli, C. Nunez and I. Papadimitriou,The warped, resolved, deformed conifold gets flavoured,Nucl. Phys. B843(2011) 1 [1004.4638]

  32. [32]

    Caceres, C

    E. Caceres, C. Nunez and L.A. Pando-Zayas,Heating up the Baryonic Branch with U-duality: A Unified picture of conifold black holes,JHEP03(2011) 054 [1101.4123]

  33. [33]

    Elander, J

    D. Elander, J. Gaillard, C. Nunez and M. Piai,Towards multi-scale dynamics on the baryonic branch of Klebanov-Strassler,JHEP07(2011) 056 [1104.3963]

  34. [34]

    Elander and M

    D. Elander and M. Piai,On the glueball spectrum of walking backgrounds from wrapped-D5 gravity duals,Nucl. Phys. B 871(2013) 164 [1212.2600]

  35. [35]

    Elander and M

    D. Elander and M. Piai,Glueballs on the Baryonic Branch of Klebanov-Strassler: dimensional deconstruction and a light scalar particle,JHEP06(2017) 003 [1703.10158]

  36. [36]

    Elander and M

    D. Elander and M. Piai,Calculable mass hierarchies and a light dilaton from gravity duals,Phys. Lett. B772(2017) 110 [1703.09205]

  37. [37]

    Candelas and X.C

    P. Candelas and X.C. de la Ossa,Comments on Conifolds,Nucl. Phys. B342(1990) 246

  38. [38]

    Superconformal field theory on three-branes at a Calabi-Yau singularity,

    I.R. Klebanov and E. Witten,Superconformal field theory on three-branes at a Calabi-Yau singularity,Nucl. Phys. B 536(1998) 199 [hep-th/9807080]

  39. [39]

    Klebanov and A.A

    I.R. Klebanov and A.A. Tseytlin,Gravity duals of supersymmetric SU(N) x SU(N+M) gauge theories,Nucl. Phys. B 578(2000) 123 [hep-th/0002159]

  40. [40]

    Papadopoulos and A.A

    G. Papadopoulos and A.A. Tseytlin,Complex geometry of conifolds and five-brane wrapped on two sphere,Class. Quant. Grav.18(2001) 1333 [hep-th/0012034]

  41. [41]

    Bianchi, D.Z

    M. Bianchi, D.Z. Freedman and K. Skenderis,Holographic renormalization,Nucl. Phys. B631(2002) 159 [hep-th/0112119]

  42. [42]

    Lecture Notes on Holographic Renormalization

    K. Skenderis,Lecture notes on holographic renormalization,Class. Quant. Grav.19(2002) 5849 [hep-th/0209067]

  43. [43]

    Papadimitriou and K

    I. Papadimitriou and K. Skenderis,AdS / CFT correspondence and geometry,IRMA Lect. Math. Theor. Phys.8(2005) 73 [hep-th/0404176]

  44. [44]

    Casalderrey-Solana, H

    J. Casalderrey-Solana, H. Liu, D. Mateos, K. Rajagopal and U.A. Wiedemann,Gauge/String Duality, Hot QCD and Heavy Ion Collisions, Cambridge University Press (2014), 10.1017/9781009403504, [1101.0618]

  45. [45]

    Charged AdS Black Holes and Catastrophic Holography

    A. Chamblin, R. Emparan, C.V. Johnson and R.C. Myers,Charged AdS black holes and catastrophic holography,Phys. 32 Rev. D60(1999) 064018 [hep-th/9902170]

  46. [46]

    Holography, Thermodynamics and Fluctuations of Charged AdS Black Holes

    A. Chamblin, R. Emparan, C.V. Johnson and R.C. Myers,Holography, thermodynamics and fluctuations of charged AdS black holes,Phys. Rev. D60(1999) 104026 [hep-th/9904197]

  47. [47]

    Gubser,Thermodynamics of spinning D3-branes,Nucl

    S.S. Gubser,Thermodynamics of spinning D3-branes,Nucl. Phys. B551(1999) 667 [hep-th/9810225]

  48. [48]

    Cai and K.-S

    R.-G. Cai and K.-S. Soh,Critical behavior in the rotating D-branes,Mod. Phys. Lett. A14(1999) 1895 [hep-th/9812121]

  49. [49]

    Phases of R-charged Black Holes, Spinning Branes and Strongly Coupled Gauge Theories

    M. Cvetic and S.S. Gubser,Phases of R charged black holes, spinning branes and strongly coupled gauge theories,JHEP 04(1999) 024 [hep-th/9902195]

  50. [50]

    Cvetic and S.S

    M. Cvetic and S.S. Gubser,Thermodynamic stability and phases of general spinning branes,JHEP07(1999) 010 [hep-th/9903132]

  51. [51]

    Kim, S.-J

    K.-Y. Kim, S.-J. Sin and I. Zahed,Dense hadronic matter in holographic QCD,J. Korean Phys. Soc.63(2013) 1515 [hep-th/0608046]

  52. [52]

    Horigome and Y

    N. Horigome and Y. Tanii,Holographic chiral phase transition with chemical potential,JHEP01(2007) 072 [hep-th/0608198]

  53. [53]

    Kobayashi, D

    S. Kobayashi, D. Mateos, S. Matsuura, R.C. Myers and R.M. Thomson,Holographic phase transitions at finite baryon density,JHEP02(2007) 016 [hep-th/0611099]

  54. [54]

    Mateos, S

    D. Mateos, S. Matsuura, R.C. Myers and R.M. Thomson,Holographic phase transitions at finite chemical potential, JHEP11(2007) 085 [0709.1225]

  55. [55]

    Nakamura, Y

    S. Nakamura, Y. Seo, S.-J. Sin and K.P. Yogendran,A New Phase at Finite Quark Density from AdS/CFT,J. Korean Phys. Soc.52(2008) 1734 [hep-th/0611021]

  56. [56]

    Karch and A

    A. Karch and A. O’Bannon,Metallic AdS/CFT,JHEP09(2007) 024 [0705.3870]

  57. [57]

    Bigazzi, A

    F. Bigazzi, A. Caddeo, A.L. Cotrone and A. Paredes,Fate of false vacua in holographic first-order phase transitions, JHEP12(2020) 200 [2008.02579]

  58. [58]

    F.R. Ares, M. Hindmarsh, C. Hoyos and N. Jokela,Gravitational waves from a holographic phase transition,JHEP21 (2020) 100 [2011.12878]

  59. [59]

    Y. Bea, J. Casalderrey-Solana, T. Giannakopoulos, D. Mateos, M. Sanchez-Garitaonandia and M. Zilh˜ ao,Bubble wall velocity from holography,Phys. Rev. D104(2021) L121903 [2104.05708]

  60. [60]

    Bigazzi, A

    F. Bigazzi, A. Caddeo, T. Canneti and A.L. Cotrone,Bubble wall velocity at strong coupling,JHEP08(2021) 090 [2104.12817]

  61. [61]

    Henriksson,Black brane evaporation through D-brane bubble nucleation,Phys

    O. Henriksson,Black brane evaporation through D-brane bubble nucleation,Phys. Rev. D105(2022) L041901 [2106.13254]

  62. [62]

    F.R. Ares, O. Henriksson, M. Hindmarsh, C. Hoyos and N. Jokela,Effective actions and bubble nucleation from holography,Phys. Rev. D105(2022) 066020 [2109.13784]

  63. [63]

    F.R. Ares, O. Henriksson, M. Hindmarsh, C. Hoyos and N. Jokela,Gravitational Waves at Strong Coupling from an Effective Action,Phys. Rev. Lett.128(2022) 131101 [2110.14442]

  64. [64]

    Morgante, N

    E. Morgante, N. Ramberg and P. Schwaller,Gravitational waves from dark SU(3) Yang-Mills theory,Phys. Rev. D107 (2023) 036010 [2210.11821]

  65. [65]

    Y. Bea, J. Casalderrey-Solana, T. Giannakopoulos, A. Jansen, S. Krippendorf, D. Mateos et al.,Spinodal Gravitational Waves,2112.15478

  66. [66]

    Y. Bea, J. Casalderrey-Solana, T. Giannakopoulos, A. Jansen, D. Mateos, M. Sanchez-Garitaonandia et al.,Holographic bubbles with Jecco: expanding, collapsing and critical,JHEP09(2022) 008 [2202.10503]

  67. [67]

    Y. Bea, R. Jimenez, D. Mateos, S. Liu, P. Protopapas, P. Taranc´ on-´Alvarez et al.,Gravitational duals from equations of state,JHEP07(2024) 087 [2403.14763]

  68. [68]

    Y. Bea, J. Casalderrey-Solana, D. Mateos and M. Sanchez-Garitaonandia,Hydrodynamics of Relativistic Superheated Bubbles,2406.14450

  69. [69]

    Y. Bea, M. Giliberti, D. Mateos, M. Sanchez-Garitaonandia, A. Serantes and M. Zilh˜ ao,Bubble dynamics in a QCD-like phase diagram,2412.09588

  70. [70]

    Witten,Cosmic Separation of Phases,Phys

    E. Witten,Cosmic Separation of Phases,Phys. Rev. D30(1984) 272

  71. [71]

    Gravitational Radiation from First-Order Phase Transitions

    M. Kamionkowski, A. Kosowsky and M.S. Turner,Gravitational radiation from first order phase transitions,Phys. Rev. D49(1994) 2837 [astro-ph/9310044]

  72. [72]

    Allen, inLes Houches School of Physics: Astrophysical Sources of Gravitational Radiation (1996) pp

    B. Allen,The Stochastic gravity wave background: Sources and detection, inLes Houches School of Physics: Astrophysical Sources of Gravitational Radiation, pp. 373–417, 4, 1996 [gr-qc/9604033]

  73. [73]

    Gravitational Waves From a Dark (Twin) Phase Transition

    P. Schwaller,Gravitational Waves from a Dark Phase Transition,Phys. Rev. Lett.115(2015) 181101 [1504.07263]

  74. [74]

    Croon, V

    D. Croon, V. Sanz and G. White,Model Discrimination in Gravitational Wave spectra from Dark Phase Transitions, JHEP08(2018) 203 [1806.02332]

  75. [75]

    Stochastic Gravitational Wave Backgrounds,

    N. Christensen,Stochastic Gravitational Wave Backgrounds,Rept. Prog. Phys.82(2019) 016903 [1811.08797]

  76. [76]

    Maldacena,Wilson loops in large N field theories,Phys

    J.M. Maldacena,Wilson loops in large N field theories,Phys. Rev. Lett.80(1998) 4859 [hep-th/9803002]

  77. [77]

    Rey and J.-T

    S.-J. Rey and J.-T. Yee,Macroscopic strings as heavy quarks in large N gauge theory and anti-de Sitter supergravity, Eur. Phys. J. C22(2001) 379 [hep-th/9803001]

  78. [78]

    Brandhuber, N

    A. Brandhuber, N. Itzhaki, J. Sonnenschein and S. Yankielowicz,Wilson loops in the large N limit at finite temperature, Phys. Lett. B434(1998) 36 [hep-th/9803137]

  79. [79]

    Brandhuber, N

    A. Brandhuber, N. Itzhaki, J. Sonnenschein and S. Yankielowicz,Wilson loops, confinement, and phase transitions in large N gauge theories from supergravity,JHEP06(1998) 001 [hep-th/9803263]. 33

  80. [80]

    Brandhuber and K

    A. Brandhuber and K. Sfetsos,Wilson loops from multicenter and rotating branes, mass gaps and phase structure in gauge theories,Adv. Theor. Math. Phys.3(1999) 851 [hep-th/9906201]

Showing first 80 references.